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Conference Paper: New formulations for evaluating hypersingular and strongly singular integrals in electromagnetic integral equations

TitleNew formulations for evaluating hypersingular and strongly singular integrals in electromagnetic integral equations
Authors
Issue Date2010
Citation
2010 Ieee International Symposium On Antennas And Propagation And Cnc-Usnc/Ursi Radio Science Meeting - Leading The Wave, Ap-S/Ursi 2010, 2010 How to Cite?
AbstractElectromagnetic (EM) integral equations include the singular integral kernels related to the Green's function. For surface integral equations (SIEs), there are two kinds of kernels, i.e. the L operator and K operator. The L operator is the dyadic Green's function which includes a double gradient operation on the scalar Green's function that results in 1/R 3 hypersingular integrals (HSIs), where R is the distance between a source point and an observation point or field point. However, the HSIs could be reduced to 1/R weakly singular integrals (WSIs) in the method of moments (MoM) solutions if divergence conforming basis function like the Rao-Wilton-Glisson (RWG) basis function is used as an expansion and testing function. Without the help of these basis functions, we must carefully handle the HSIs and this happens in the implementation of Nystr̈om method (NM) or boundary element method (BEM). The K operator includes a single gradient operation on the scalar Green's function, yielding 1/R 2 strongly singular integrals (SSIs) in the matrix elements. The SSIs also exist in the L operator in the MoM when the RWG-like basis functions cannot be used as a testing function. The accurate and efficient evaluation for the HSIs and SSIs is essential in solving the SIEs because they have a significant impact on the numerical solutions. © 2010 IEEE.
Persistent Identifierhttp://hdl.handle.net/10722/183030
References

 

DC FieldValueLanguage
dc.contributor.authorTong, MSen_US
dc.contributor.authorChew, WCen_US
dc.date.accessioned2013-05-02T05:18:10Z-
dc.date.available2013-05-02T05:18:10Z-
dc.date.issued2010en_US
dc.identifier.citation2010 Ieee International Symposium On Antennas And Propagation And Cnc-Usnc/Ursi Radio Science Meeting - Leading The Wave, Ap-S/Ursi 2010, 2010en_US
dc.identifier.urihttp://hdl.handle.net/10722/183030-
dc.description.abstractElectromagnetic (EM) integral equations include the singular integral kernels related to the Green's function. For surface integral equations (SIEs), there are two kinds of kernels, i.e. the L operator and K operator. The L operator is the dyadic Green's function which includes a double gradient operation on the scalar Green's function that results in 1/R 3 hypersingular integrals (HSIs), where R is the distance between a source point and an observation point or field point. However, the HSIs could be reduced to 1/R weakly singular integrals (WSIs) in the method of moments (MoM) solutions if divergence conforming basis function like the Rao-Wilton-Glisson (RWG) basis function is used as an expansion and testing function. Without the help of these basis functions, we must carefully handle the HSIs and this happens in the implementation of Nystr̈om method (NM) or boundary element method (BEM). The K operator includes a single gradient operation on the scalar Green's function, yielding 1/R 2 strongly singular integrals (SSIs) in the matrix elements. The SSIs also exist in the L operator in the MoM when the RWG-like basis functions cannot be used as a testing function. The accurate and efficient evaluation for the HSIs and SSIs is essential in solving the SIEs because they have a significant impact on the numerical solutions. © 2010 IEEE.en_US
dc.languageengen_US
dc.relation.ispartof2010 IEEE International Symposium on Antennas and Propagation and CNC-USNC/URSI Radio Science Meeting - Leading the Wave, AP-S/URSI 2010en_US
dc.titleNew formulations for evaluating hypersingular and strongly singular integrals in electromagnetic integral equationsen_US
dc.typeConference_Paperen_US
dc.identifier.emailChew, WC: wcchew@hku.hken_US
dc.identifier.authorityChew, WC=rp00656en_US
dc.description.naturelink_to_subscribed_fulltexten_US
dc.identifier.doi10.1109/APS.2010.5561064en_US
dc.identifier.scopuseid_2-s2.0-78349253501en_US
dc.relation.referenceshttp://www.scopus.com/mlt/select.url?eid=2-s2.0-78349253501&selection=ref&src=s&origin=recordpageen_US
dc.identifier.scopusauthoridTong, MS=11839685700en_US
dc.identifier.scopusauthoridChew, WC=36014436300en_US

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